The Conformal Group of a Conformally Flat Space Time and Its Twistor Representations

  • Ivan T. Todorov
Part of the Trieste Notes in Physics book series (TRIESTE)

Abstract

Let (M,g) and (’M,’g) be two D-dimensional real pseudo-Riemannian manifolds, whose metric tensors g and ‘g have the same signature. A diffeomorphism φ: U →’U of a neighbourhood U ⊂M onto ‘U⊂’M is said to be conformal if the corresponding tangent map φT preserves the angles. In a slightly more technical language this means that for given coordinates Xµ and ’Xµ on U and ’U we have
$$\frac{{\partial \varphi _{(x)}^\kappa }}{{\partial {x^\mu }}}\frac{{\partial \varphi _{(x)}^\lambda }}{{\partial {x^\nu }}}'{g_{\kappa \lambda }}(\varphi (x)) = {\Omega ^2}(x){g_{\mu \nu }}(x)(\Omega > 0).$$
(1.1)

Keywords

Minkowski Space Conformal Transformation Conformal Group Twistor Representation Causal Order 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer-Verlag Berlin Heidelberg 1986

Authors and Affiliations

  • Ivan T. Todorov
    • 1
    • 2
  1. 1.Scuola Internazionale Superiore di Studi AvanzatiTriesteItaly
  2. 2.Institute for Nuclear Research and Nuclear EnergyBulgarian Academy of SciencesSofiaBulgaria

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